Restoring device for locking circuits



Filed April 4, 1946 OUTPUT 7('0 07'l/FR lOCK/NG CIRCUIT A5 I F/6'.3) OR 70 OTHER UTILIZATION MEANS July 11, 1950 m ur r No/E 4 SPACE. m uzss CIRCUIT 3 UNEX MARK \LREsmR/A/a PM:

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g E 2 60 WORD PER MINUTE 7 3 I I I I 7wv/r TELETYPEWR/TER TIMING '44 132 207295370 458' 0 as I63 325 4/4 489 TIME MILL [SECONDS E. MITCHELL ATTORNEY lNVENTOR J C J. C. E. MITCHELL I RESTORING DEVICE FOR LOCKING CIRCUITS 2 Sheets-Sheet 1 g I g IMRY/Al' MAM/7110f T R2 PULSE sue/,

w v2 TELEGRAPH) SIG/VAL l u a: INPUT 'WW- -ww- I o 1L: \IO R3 R4 1 s1 51 g Y 4 i atented I1 RESTORING DEVICE FOR/ LOOKING CIRCUITS John 0. E. Mitchell, Montreal, Quebec, crimes. assignor to Radio Corporation of America-,- a

corporation of Delaware Application April 4, 1946, Serial No. 659,477

In this application I diSCIOSe improved circuits of the type having two conditions of stability known in the radio and allied arts as a, locking circuit or triggering circuit or flip-flop circuit. The circuit involved may be of the general type disclosed in Finch U. S. Patent #1344350, and is of wide use in the radio art.

These locking circuits have two electron dis charge systems with their electrodes so coupled that when one discharge system starts to draw current, current is switched through said one system and cut oil in the other tube, and this condition of stability remains until something takes place to start current through the said other discharge system so that current is switched therefrom and cut oil in the first system. This second condition of stability remains until something takes place toreestablish the first condition. Usually the locking circuits are controlled by application of a, potential of pulse energy either alternating current or direct current of varying magnitude to an electrode of one or both discharge systems. The output of the locking circuit, which is considerably stronger than the control potential and is of better wave form may be used as desired. In a particular application the locking circuit output is used in a telegraphy system to operate a, tone keyer or a teletypewriter or other recording means. Such an arrangement is disclosed in my U. S. application Serial #670,085, filed May 16, 1946, now Patent #2,50'7,730, dated May 16, 1950, and in Cohoon abandoned U. S. application Serial #649,343, filed February 21, 1946. In these systems in order to derive strong signals of improved wave form a locking circuit or two locking circuits in cascade are controlled by pulse energy representing sig nals. The locking circuits are triggered between their two conditions of stability in accordance with signals and a potential is taken from the locking circuit output and used. to operate a teletypewriter or tone keyer or other recording apparatus. The control pulses for the locking circuit may be derived from on and off telegraphy transmission or on-ofi facsimile transmission or from frequency shift telegraphy signals or facsimile signals. In both these types of signals at the receiver detection takes place to derive pulse energy the magnitude of which varies usually between two values, (may be of reversible polarity), one representing marking condition, the other representing spacing condition.

In telegraphy systems of this type the transmission is synchronized with the receiving mechanism to this extent. The transmission usually 7 Claims. (Cl. 178-70) iii) ends in the marking condition so that the 'rceiver output pulse energy at the end of the mes sage, and between elements of a message'and letters of a message, is of a magnitude such'as to represent the marking condition. When the received signals are used to operate a teletype writer directly or through tone keyers the teletypewriter mechanism obviously should also be arranged to stop operation after excitation by pulse energy representing the marking condition and to start operation on receipt of pulse energy of the magnitude representing space condition in the telegraphy system. The locking circuit, as stated above, is controlled between its two conditions of stability by the received signals and its operation is so related to the teletypewriter and to the signal pulse magnitude that it is left in one condition of stability by reception of pulse energy of a magnitude representing marking condition and in the other condition of stability on reception of pulse energy of a magnitude representing space signal condition. In practice at the termination of a message or between letters or signal elements the locking cir cuit may for some reason be left in the mark condition, or, may be tripped to the space condition by pulse energy resulting from static inter.- ference or from noise developed in the transmitter or receiver. Then the locking circuit is left in space condition instead of in mark condition, as desired. In the seven unit code system now in wide use in the radio art the first code element starts the typewriter distributor. The next five signal elements are for message purposes and the seventh signal element stops the distributor. Moreover, the teletypewriter distributor is started each time a signal character representing space is sent and is stopped usually by a stop character representing mark which is sent, but it may be arranged to stop itself. In any event, the distributor started by a space condition in the locking circuit must go a complete cycle before it is stopped. Now since a noise element representing space has tripped the look ing circuit to space condition, the teletypewriter distributor will race or start rotating at a fixed speed. Once it is started it must complete'a revolution before it is stopped. If the locking circuit is still on space the distributor will again start and repeat its cycle. The system is then out of control as far as the operator is concerned. Obviously no recording or improper recording takes place and the printer will race untila pulse of a magnitude representing marking condition is received on the system and applied to the locking circuit to trip the same to mark condition and then the printer-distributor will come to rest and remain in a quiescent condition until a signal again trips the locking circuit to the space condition.

The object of the present invention is to provide in looking circuits of this general type means to return or restore the locking circuit to the mark condition in the event that it is either left on space at the conclusion of a teletype signal or that a noise burst, in the absence of teletyp'e signal, trips the locking circuit to space by un wanted or spurious noise energy resulting in pulse energy of a magnitude sufiicient to actuate the locking circuit. Means is also included for delaying this restoring action so that the restoring action does not interfere with normal signalling, i. e., does not take place quickly enough to be operated by space characters making up the signal. The mark return circuit of, the present invention provides a pulse to returnfthelocking circuit, to mark condition shortly after the unwanted pulse is received. My 'in vntion serves substantially thesame purpose asthe locking circuit; restoring means, of Atwood e tlal. U. S. application Serial #618,769, filed September 26, 1945. Of course in both cases a carrier is assumed to be present, although it may have faded severely.

' 'In'so'me prior locking circuit restoring arrangements' tube means and circuit element connections are also used to restore the locking circuit to one of its conditions of stability. However, in; these arrangements two factors control the operation of the restoring circuit. One is the space teletype signal or, in its absence, space directed noise, and the other ,is the condition of thelocking circuit. It maybe seen thatcontrol of the restoring circuit by space directed n oise can be a distinct disadvantage. The space directednoise pulses disable (bias off) the restoring circuit in the same way as do space signals, so that-in the case where there are a succession oi space directed noise pulses it'is necessary that the restoring tube waituntil this accumulated bias ha's leaked offi before it can trip the locking circuit to mark. Furthermore, it is necessary thatthe charges from a previous teletype signal 1e" off before the restoring circuit can operate o n the receipt of a new space directed noise. Furthermore, it is extra sensitive to the first space signal, and this sensitivity also enhances th'tpossibility of the locking circuitbeing tripped ln'resp'ons'e to a'space directed noise pulse.

A further object of my invention'is to provide an improved but simple means'for restoring the lccking' circuit to one condition of stability wherein there is only one factor controlling the operation of the mark return'circuit andthat is the 'condition of the locking circuit (mark or space) Should the locking circuit be tripped to space the restoring circuit immediately comes o effect, and if thelocking circuit remains on space for the prescribed length of time the restoring circuit will trip the locking circuit back tcmark. This exactly fulfills the'object of the invention.

In the description givenabove and in the description which follows it is assumed that the transmitted signal ends on mark and that the locking circuit then is in a particular condition of stability andthat the printer distributor is started by a space condition} It will be obvious thatthe inventionis equally applicable if the transmission is caused teend onspace and the 4 printer starts on mark. Obvious changes such as reversal of the locking circuit response, etc., are then made.

In describing my invention in detail reference will be made to the attached drawings wherein Fig. 1 illustrates by circuit element and circuit element connections an embodiment of a locking circuit with restoring means arranged in accordance with my invention;

Figs. 2 and 3 illustrate modifications of the arrangement of Fig. 1 and Fig. l illustrates by voltage time curves the operation of my improved trigger restoring circui In thedrawings, tubes or electron control devices V! and V2; are connected in a locking circuit. In this circuit the anode of tube electron discharge device V! is coupled to the screen grid. of electron discharge device V2, while the anode of tube V2 is coupled to the screen grid ofv tube VI. The anodes. of tubes Vi and V2 are connected by resistors R], and R2 respectively to the positive" terminal of a source of potential the negative terminal of which is grounded. The tubesjhave'their cathodes tied together and connected to, groundby a resistance R3; The suppressor grids are connected to the cathodes. The circuit as described is in principle as disclosed in Shenk abandoned U. S. applicationSerial #580,525, filed March 2, 1945. The arrangement is such that when the potential on the control grid o'ffsay tube V2 is made mor positive'current starts to flow in tubeVi and the potential at-the andde'of tube V2 drops so that the potential onthescreen grid of tube Vi becomes less pdsitivetoreduce current flow in tube V! and" the actionfis cumulative to the extent that 'tube"current -flow is all switched through the tube V 2; and; cutoff-in the tube VI. The locking" circuit} is then in "one of its conditi'oris 'ofstability and remains there until, for some reason, 'u'suall-y application'of a, potential toan electrode of'one of the tubes, starts the current to flow in VI or reduces current flow in V Z so that'the action described above is repeated in a reverse sense ftorswitch. the current all through tubeVl and cut off current flow in tube V2.

' Thelocking circuitsas describedabove are of wide application inrthe; radio. art. The. lockin circuits are particularly applicable to telegraphy signalling andiare put to many uses in the telegraphy art; For example, they are used between the telegraphy receii/er demodulators and the recording apparatus. The locking circuit is then excited by thetelegraphy'signals' taken from the output. of! the. demodulator and; operates the 'recorder either. substantially direetlyjor by. way of a tone keyer. In some 'casestwo locking circuits are cascaded. Two examples of such use are shown in Schockettal. U'. S. application Serial #632,978, filed December 5, 19%,, and in Peterson etal. application Serial .No. 629,298, filed November 17, 1945, now Patent #2,494l,309, dated J anuary 10, 1950. When so used tel'egraphy signals may be impressedion'the tern'linals land may be of the wave form shown over. the input leads. Since they are obtained by rectifying frequency shiftedcurrents of intermediate frequency or keyed-telegraphy'signals they. may include undesired components in" whichfcase. they may be passed through 'afi lter. 2!! to remove therefrom alternating componentsiof' frequency higher than the keying frequencies. They are'then' supplied to a relatively large capacitor C3. and. fed from crate. signal recording apparatus. it may be usedas disclosed in Cohoon U. S. application Serial #649,343, filed February 21, 1946, to

scribed above, i. e., ina normal manner.

' changes with reference to a base value. "the switch SI is closed the gas discharge tube i the capacitor C3 through a resistor R to the control grid'of tube V2; The control grid: of tube V2 is biased as desired by a resistor R4 connecting the control grid tov ground. The v'ar'yingpulses -at..I0 operate as described above on the control grid of tube V2 to make the same. conductive or non-conductive thereby also-makingtube VI non- .conductive or. conductive. The output may be taken from various points in thelocking circuit.

;-In the embodiment shown the output leads are is a potential which varies between two substantially fixed values in accordance with signals. This potential may be utilized .as desired to op- For example,

control the potential on the grid of one of the tubes of a second locking stage which in turn operates ,a teletypewriter relay.

In order to simplify the description it will be assumed that in mark condition the tube VI is conductive and tube V2 is non-conductive, and that in space condition tube VI. is non-conductive and tube V2 is conductive. It will be understood, however, that these conditions of stability of the system may be changed as desired. Furthermore, it will be assumed that the signal transmission ends on mark condition so that the pulses at the input I0 are negativeand of. a magnitude such as to trip the tube V2 to a non-conductive state, i. e., on mark condition the signal is more negative than on space condition. It is further assumed that signal transmission starts on space.

If after a mark pulse has been applied to the control grid of tube V2 to trip the circuit into marking condition of stability with tube VI conductive, noise or static produces at the input ID a. pulse which is of a magnitude such as represents spacing signal, the tube V2 is made conductive and tube VI non-conductive, i. e., the system will be tripped to the space condition instead of the mark condition. The gist of my invention is means for restoring the locking circuit to the mark condition in the event static or noise energyhas tripped this circuit to space condition. This means comprises an electron discharge voltage regulator device V3 which may have its cathode electrode connected to ground and thereby to the cathodes of tubes VI and'V2 and its anode electrode connected by resistor R6 through a pedance of this gas tube is shunted by condenser CI and the anode of this tube is coupled by a condenser C2 and another contact of the switch SI to the control grid of the tubeV2.

In operation with switch SI in the open position as shown the locking circuit operates as de- This locking circuit will lock on either mark or space,

- depending on the magnitude of the incoming signal pulses until a signal pulse of the opposed polarity is received. By opposed polarity applicant includes any signal the magnitude of which Now if 'the high potential direct current source and across the anodeto ground impedance of tube -V I.

The breakdown potential of the tube V3.19 of a value intermediate the potentials appearing at I the anode end of resistance RI in'the two difi'erent conditions of stability of the lockingcircuit, i. e., when tube VI is conductive and when tube VI is non-conductive. In an embodiment operated the breakdown potential of the tube V3 is approximately volts D. 0., and the voltage drop across the tube V3, 1. e., between its anode andground is equal to about 75 volts D.'C. whe the'tube is fully conductive. I

Recall that in mark condition tube VI is conductive and the potential at its anode is low. say 20 volts, and that this is the mark condition at which the locking circuit is supposed to come to rest. Static or other noise may then trip the locking circuit so that the tube VI becomes nonconductive and the voltage at the plate 01 tube VI and the screen grid of tube V2 rises and reaches a positive value above the breakdown voltage of tube V3, say volts positive. If the locking circuit rests on space for an appreciable length of time condenser CI then charges up to a potential suiiicient to breakdown tube V3, 1. e., charges up to about 105 volts. The potential across tube V3 drops substantially instantaneously to say 75 volts positive, which-is the drop across the tube V3 when it is fully conductive. This sudden drop in potential at theanode end of tube V3 applies through condenser C2 and switch SI to the control grid of tube V2, a pulse of energy which is negative and of a magnitude sufficient to reduce current flow in the tube V2 and start the tripping or looking action described above to switch the current through VI and cut ofi current in tube V2. In other words, the pulse of potential developed across tube V3 when the same breaks down and applied to the grid of tube VI, trips the locking circuit to the mark condition at which it is to rest at the end of a message or between signal elements. Under the mark condition the voltage at the plate of tube VI and at the screen grid of tube V2 is low, say only about 20 volts. Tube V3 which became conductive, has drained off the charge, from condenser CI to the point at which tube V3 becomes non-conductive. The mark condition restoring tube V3 and its connections are then again ready to restore the circuit to mark condition if the same is tripped to the space condition by unwanted pulses and remains in the space condition for a period of time greater than that which elapses between. mark and space during normal signal conditions.

My mark return circuit V3 and components: may be considered as a relaxation oscillator which: is supplied with adequate voltage for its opera-- tion if the locking circuit remains on space The first pulse of the relaxation oscillation, being:

fed to the grid of the locking circuit, restoresthei looking circuit to mark and disables the oscillator. V3 and components may also be considered as a form of relaxation oscillator when sufficient noise is present to tend to keep the lockin circuit on space. In this case it will continue to produce new mark pulses at approximately its relaxation oscillation rate until the noise ceases. Because this mark return circuit takes the form of an oscillator it is possible to adjust its relaxation time in such a way that it does not cause the teletype to print a character when the locking circuit is returned tqmark following a space directed noise pulse. This .is l the case if the locking circuit is returned to mark noise pulses of a space sense.

eircuit tried out space noise-pulses occurring im- 1525i:- s one iduringgza stop interval on the teletypwriter. This shown in Fig. 4.

The valuesofRfi and CI to the breakdown voltage of tube VS-so that condenser C-l will not charge to the breakdown .voltage during the longest space which normally exists during telegraphy transmission. 7 This is of the order of 125 milliseconds. The time constantof Cl and Rfi is chosen to be about 220 milliseconds to allow for a partial chargeoi the are choseninarelation' condenser C! during normal telegraphytrans- .mission. During normal transmission of teletgpesignals the average voltage across 0;] :is less circuits is that this circuit cannot be rendered temporarily inoperative by rapidly successive 'In one restoring .inediately after the mark returncircuit has func- .tioned, .could by returning the locking-circuit to .space condition render the mark return circuit temporarily inoperative. My improved circuit :op-

crates :directly after each appearance of :one or .a .suocession of pulses representing space condition of :a duration greater than approximately 125 milliseconds.

The arrangement-of Fig. 1 may be modified as illustrated in Fig. 2. In the embodiment of Fig. 2 .the tube V3 is a gas thyratron and is in .a circuit which is'broadly-similar to the arrangement of Fig. land may be considered a relaxation oscillator set into operation on application to the locking tube circuitof a pulse of energy .of tube V2. The drop in potential across the tube V3 is applied over condenser CI through condenser C2 and switch SI to the grid ofitube V2, and is in a negative'direction and of sufiicient magnitude to havethesame-efiect as application of-a marking pulse to this grid to trip ltheilocking circuit to marking condition'whereat tube V2 is non-conductive and tube VI is com ductive. In operation then oscillation takes .place oris permitted in the relaxation oscillator including tube V3 when-its plate voltage rises to a value which allows plate current to flow. The .plate voltage rises when tube V! is non-con ductive for a period of time greater than-that .rneasured by marking elements .in a normal signal. The grid bias of tube V3 applied by source 20 determines or measures the magnitude of the plate voltage at which currentwill flow in tube V3. The condenser Cl, as in the embodiment of Fig. .1, measures the time necessary for :application of voltage before the tube V3 becomes conductive. Operation is otherwise similar to that of-the tube V3 in Fig. .1.

. The potential applied to resistance RBrmay be .obtained from otherpoints than the plateof tube VI and the screen of tube V2. For example, this gootentialmay be derived 'from aproper cathode resistor, for example, resistance-40 of Fig.3,in ;jthe .second.. l ocking .circuit driven .by the locking terminal of the source;

circuit shown. "The voltage is -tselected .froni'ia :point where a voltage greater than the :breakdown voltage :of tube V3 is available. .If the :polarity of the voltage -:applied to the "resistor 5R6 is:negative, as might be the case in some applications, :62 may then be :connected to the .gridbf tub-eVl by liftingthe grid of atube'vtl ofi ground direct current potential and returningv it to Jgroundthrough asuitable 'resistor. vThis ofzcourse *requ'ires. reversal of the polarityof tube V3. "Then when the undesired pulse has tripped the circuit to space condition afteran adjustable period :of time the condenser =CI charges and tube "V3 breaksdown and the high negative potential 'on :its :cathode drops'to be less negative and a rising 'potential'issapplied to'the grid of tube 'V'l 'to turn it on thereby tripping the entire system to "the mark condition as desired.

Another version is 'to introduce airesistor in series with the grounded terminal of tube V3 and connectthe "junction point of tube V3 and 'the said resistor directly or through a condenser resistor combination to the grid of tube V2. This embodiment may be as illustrated in Fi 3.

Such an arrangement is illustrated in Fig. 3 of the drawings. In-this embodiment the tubes V! and V2 are connected and operated substantially 'as described h'ereinbefore .in connection with Figs. 1 and 2. Asecondilocking circuit including tubes V4 and V5 is driven "by voltages derived from the first locking circuitincluding tubes VI and V2. Totdo this the control grid of tube Vii is connected by a resistor '25 .and condenser cs to the anode of tube V2 and screen grid of tube VI. The locking circuit including tubes Vtv and V5 is substantially as described in Cohoon U. S. application Serial '#64a9,343,jfi18d February 121,, 1946. Separate anode sources are used for the two tubes. The anode circuit of tube vs runs :irom the positive terminal ofthe mark source through the tube :tothe :tubercathode and thence by lead .28 to the :teletypewriter or similar recordercoupledto the leads 3E! and-back through switch S3 and resistor :32 to the negative The potential drop .developed'in.theresistance 32 is applied to the accutrolgrid of tube V5 by resistor 36 to cutthistube off in the usuallocking circuit fashion when tub V4 is :conductive. a

The anode direct current circuit of the :tube V5 :fiows from the .positive terminal of the space source to the anode of tube V5 and irom its .cathode by lead 38 and switch S3 through the .teletypewritericonnectedto terminals 30 (in the opposite direction) backthrough the resistor to the negative-terminalof the fspacezsource or space battery. The potential drop developed .in the resistor-401s applied byeresistor 42'to theagrid of the tube V4 when tube V5 is conductive to cut off tube V4 in the usualvlocking .circuitfashion. Since the tube V2 is non-conductive onrmark, i.e., has its :maximum anodepotential, the tube V4 whichhas its grid excited by this anode .potential is conductive on mark,.-and its plate source .has been designated the marking source because current supplied thereby runs through the .recordingrapparatus to operate the same. The tube V5 is-then .nonj-conductive. Whenthe tube V-Zis conductive, i.e., in the "space condition, tube V4 is non-conductive and tube Viisconductive and the plate source for this tubeis designated .thespace-sourcebecause then currentfrom this source runs in the opposite direction through the ,recordingcircuits. Theswitch S3 isshown in I -what. istermed thapolar position,.-i. .e.,.in theme- 9 l sition described wherein when current flows through V4 it passes in one direction through the recording means connected to the terminals 3t, and when current flows through tube V5 it passes in the opposite direction through the recording means connected to the terminals 30. The adjustable resistance 44 is a means for adjusting the intensity of the current through the recorder.

It will be noted that when current flows in the tube V5 a potential drop is developed in the resistor 49 which is'n'egative at the point 46 and this potential drop is applied by resistor R6 to the tube V3. Current flows in the tube V5 when the locking circuit including tubes VI and V2 is in the space condition with tube V2 conductive because, as pointed out above, when V2 is nonconductive V4 is conductive, and when V2 is conductive V4 is non-conductive, making V5 conductive. which is the space condition. Moreover, the potential developed at the end of resistor All remote from the cathode of tube V5 is negative and is of a value E (with respect to ground) depending on the current in tube V5 and on the magnitude of the resistor 40. The tube V3 is then connected in reversed polarity with respect to its connections in the embodiment of Figs. 1 and 2. That is, tube V3 now has the tube V5. A negative potential E is developed acro s the resistor 40 and applied to the cathode of tube V3. The magnitude of this potential E is made suificient to exceed the breakdown potential or voltage of the tube V3. In one embodi ment the potential E is approximately 65 volts so that the-breakdown voltage of the tube V3 is made 55 volts or less. If the voltage E is present long enough to charge up condenser Cl, tube V3 breaks down to produce in resistor RID a potential drop which is inthe negative direction at the anode of the tube V3 andoperates through the condenser C2 to simulate the effect of application of a marking signal to the grid of tube V2. That is, it biases this tube to cutoff, thereby turning on tubes V! and V4 and turning off tube V5 so that both locking circuits are in the condition at which they are intended to be after the application of a marking character.

The operation. of the embodiments described hereinbefore has been further illustrated and described in Fig. 4. In Fig. 4 line X is shown as a voltage versustime curve representing what might be the noise input to the locking cir-' cuit, say to tube V2. The noise or static might generate a'pulse peak in the space signal direction, i.*e., positive and of a magnitude comparable'to a space signaL This would trip the locking circuits to the-space conditionwhich, as stated above, would prevent proper operation of the recording apparatus synchronized to start on space and end on markn The apparatus described hereinbefore then produces at V3 a negative peak of a magnitude comparable to a normal marking pulse and applies the same to the control grid of, a tube in a locking circuit to make the same efiective to trip to the marking condition, The

next line Y of Fig. 4 illustrates at P the voltage on the anode of the tube VI and screen grid of the tube V2 in the space and marking condition, and

at Q the potential generated by my locking circuit restoring arrangement at the anode of the restoring tube V3. In both graphs the ordinants are direct current voltages and the abscissas repbelieved, self- Em=mark volts Screen V2 Vf=breakdown voltage of V3 tr may be chosen so that the locking circuit K returns to mark during a stop interval on the teletypewriter. In the above case tr is approximately 470 milliseconds, in which case R6 would be 2.5 megohms and CI 0.1 mfd. approximately, with the voltages shown.

If the teletypewriter is returned to mark con-,-

dition during or very near a stop interval in its tycle it does not print a character, whereas if it," is returned at an arbitrary time it generally prints a letter which is of course undersirable.

What is claimed is; 1. In combination, a'locking circuit compris-,

ing two electron control devices having electrodes intercoupled and connected to direct current sources in such a manner that when current is cut ofi in one devicecurrent flows in the other device and vice versa, apparatus for applying potentials which vary between two magnitudes, representing signal elements to said locking circuit to trip the same back and forth between the two conditions of current conduction in the devices as the potentials vary between said mag-f.

nitudes, and means for reestablishing a stable condition of current cut oifin a predetermined one of said devices and current flow in the other,

mains tripped for a time period exceeding the,

duration of the longest signal element, comprising a relaxation oscillator including an electron discharge device in a capacitive and resistive circuit having a time constant which is longer than the time duration of the longest signal element, means responsive to current in said locking circuit for developing a potential of a magnitude suiiicient to start oscillation in said relaxation oscillator when current is turned on in said one. device and off in the said other device for a time period exceeding the time duration of the longest signal element, means forapplying said potential to said electron discharge device, and means coupling said resistive circuit to an elec'-' trode in one of said control devices to trip said locking circuit to reestablishsaid condition of current cut ofi in said one device and current flow in said other device.

2. In combination, a locking circuit comprising two electron control devices having electrodes intercoupled and connected to direct current sources in such a manner that when current is cut off in one device current flows in the other device and vice versa, apparatus for applying potentials which vary between two. magnitudes repaentoda resenting signal elements; to; said'locking circuit tudes, means.for-reestablishing-a stable condition of current. cut off in: apredetermined one of said devices-.: and current flow in. the other of said devices inthe event thelocking: circuit is: tripped from said conditiorrof stability'andi remains; tripped for a time period exceeding a predetermined time period, comprising. a gas tube in acapacitive and resistive relaxation oscillato circuit having a time constant which is longer than said selected predetermined time period, means for biasing said gas tubeto cutoff when current is cut off in said one device and for developing a potential of a magnitude sufiicient to overcome said bias when current is turned on in said one device for a time period exceeding said predetermined time period, means for applying saidpotential to said gas tube whereby the condenser of said relaxation oscillator circuit is charged and said gas-tube is made conductive, and means coupling said: resistive: 0113: cuit, to an electrode intone of said: devices to ap-- ply thereto; av potential which trips said. locking; circuit to; reestablish said condition of currentcut oli in said one device and current, flow in; said-other. device;

In a telegraphy system, a locking circuit arrangement including twoelectron control devices each having electrodes, intercoupled and; conected by impedances to.--direc.t current sources in a manner such that when current flows in one device, current is cut off. in the.- other devicev and vice: versa, a. source ofv pulse.- energy, which varies in, magnitude between twovalues, representingtwo signal, conditions, coupled to an electrode of one device to-trip the-currentback and forth between the devices as the magnitude varies between said. values, said pulse-energy representing signal elements arranged to. terminate in thesame signal condition so that one device is left inraconductivecondition and. the other device in a non-conductive condition, means forrestoring the-terminal condition of said locking circuit in the. event static or other disturbance produces a pulsawhich tripssaid locking circuit to a condition. in which said. one deviceis non-conductive andsaidnother'device is conductive and said last conditionremains for a timeperiod-whiclrexceeds a theetime period of the, signal-elements, comprising an. electron. discharge deviceshalling. a; breakdown. potential whichis intermediatev the limits. or the potential variation in oneof said impedances, a condenser in shuntto theinternalimpedance of' said. discharge device; means coupling said dis charge device to. said one impedance so that the potential developed in. said one impedance isap plied to.said discharge device, and a coupling'between an electrode.v of said discharge device and aecontrotelectrode of one of said control devices.

4. In combination, a locking circuit comprising twoitubes.eachhaving:electrodes-including a control-grid and ananode intercoupled and connected toa. direct current sourcein such a manner that whentcunrent is. out ofi'inrone-tube it flows in the othertube and.vice=versa, apparatus for, applying: potentials which vary between" two magnitudes; representing signal elements to said locking circult: to tripthesame ba-ckhand forth between the two'conditions of current conduction in the tubes. as; the'potentials vary between said. magnitudes; means for re-establishing a stable condition of current cut ofi: in. a. predetermined one of. said tubes:andtcurrent flow in the other of said tubes in the eventl-the locking circuit-is:- trippedt from said conditioner stability and remains tripped for a. time period: which is longer thanthe time duration of any signal element, comprising an electron. discharge-device with an. anode. and cathodein a: capacitive and resistive-relaxation oscillator network having a time constant which islonger than, the time duration of any signal element, a coupling between the anode of said other tube and the network for charging the condenser of said. network toa; potential of. a magnitude suficient to? make said device conductive whenv current: is turnedon in said one tube and; off in. said.- other: tube tor: a timevper-iod exceeding the time 'cluration' ct. any signalz element, and a (IOU:- pling' between: said network anda. control grid,

of saidcone tube. I

5; In, combination; a locking, circuitcomprising twotubes-- eachhaving: electrodes includingv an anode and a control grid and having their electrodes-intercoupled and. connected .toaz direct current source in such a: manner that when-currentis cut-offin. one tubei-t flows inv the other tube'and:

vice: versa, apparatus for applying potentials which vary between two magnitudesrepresenting signal. elements to said locking circuit to tripthe same back and forthv between the two conditions of current conduction in: the tubes as: the potentials:var;y betweenv said magnitudes, meansfor re-establishingastable condition: of current cut.

on inv at predetermined one of: said tubes. and: currentfiow in the. other of.v said: tubes: in the event the locking. circuit istripped: from. said. condition of stability and: remains. tripped for a period:

. of time of a duration longer. than any signal element, comprising electron discharge device having a cathode, an anode and a.- negative. con. trol grid: and. having its anode and cathode nv a capacitive. and' resistive relaxation oscillator circuit having atime constant which is longer than. the duration of any signal element; a connection including a resistance between-the anode of said.- other tube and, the anode; of: said. device for applying thereto a potential ofa magnitude sufiicient' to, make. said device conductive when: cur-- rent istur-ned on in said=one tube and: offin said other tube for a time period exceeding the duration of. any signal element, and a coupling betweensaid network and. the control gri'dof, said one: tube. V

6; Ina telegraphysystem, a; locking circuit-com prising a pair of eiectron control devices each having electrodes cross-coupled and coupled by" impedances to direct current sources such that:

; when current flows in: one: device current is out offin the other d'evice and vice versa, a source of pulse energy of varying magnitude coupled to a control electrode of one device to trip the current back and forth between the devices, as the magnitude of said source varies, said pulse en-' ergy representing signals arranged to terminate in the same pulse source magnitude so that one device is left in a non-conductive condition and the other'device in a conductive condition, means i for restoring the terminal condition of said lock a period of time which exceeds the signal pulseduration, comprising a gas discharge tube having its-'electrodesshunted by a condenser; means coupling the impedance between the electrodes of said gaseous discharge tube in shunt to a portionof saidlocking circuit whereat is developed a;

potential which is higher than the breakdown potential of said gas tube when said one device is left in a conductive condition and said other device in, a non-conductive condition, and a connection between an electrode of said gas tube and a control electrode of said one device for applying thereto when said gas tube breaks down a potential which trips said locking circuit to make said one device non-conductive and said other device conductive.

7. In a telegraphy system, a pair of locking circuits each comprising two electron discharge devices having control electrodes and anodes crosscoupled and connected by impedances to direct current sources in such a manner that when current starts to flow in one device it is cut off in the other device and vice versa, a connection between a device of one looking circuit and a device of the other locking circuit to couple the same for cascade operation, an input circuit for applying direct current potential, representing signals, which varies between two values representing different signalling conditions to a control electrode of a device in said one looking circuit to trip the same so that current flows through one device and is out off in the other device when 14 the direct current potential represents marking condition, means for restoring said one looking circuit to marking condition in the event static or other disturbance trips it to spacing condition for a time period greater than the maximum signal element time period, including an electron discharge device having electrodes shunted by a condenser and connected to an impedance in the circuit of said other locking circuit, and a connection between said last-named device and a control electrode in one of the devices of said one looking circuit.

J. C. E. MITCHELL.

REFERENCES CITED UNITED STATES PATENTS Name Date Ranger Aug. 23, 1932 FOREIGN PATENTS Country Date Great Britain Feb. 28, 1938 Number Number 

